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1 WDM WDM Piotr Turowicz Piotr Turowicz Poznan Supercomputing and Networking Center Poznan Supercomputing and Networking Center piotrek piotrek@ man.poznan.pl man.poznan.pl 9-10 October 2006 9-10 October 2006

1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center [email protected] 9-10 October 2006

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Page 1: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

1

WDMWDMPiotr TurowiczPiotr Turowicz

Poznan Supercomputing and Networking CenterPoznan Supercomputing and Networking Center

piotrekpiotrek@@man.poznan.plman.poznan.pl

9-10 October 20069-10 October 2006

Page 2: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

2

Agenda

Dense Wavelength Division Multiplexing– The traditional and emerging challenges– How does DWDM work?– What are the enabling technologies?– The evolution of optical fibres

Page 3: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

3

Optical Networking Challenges

Faster

Further

More Wavelengths

Traditional Challenges

Page 4: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

4

Optical Networking Challenges

Faster

Further

More Wavelengths

Access(FTTN, FTTC, FTTH)

Switching

Muxing

Traditional Challenges Emerging Challenges

Page 5: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

5

What is a Wavelength Mux?

Time Division

Mux

Tributaries are sent in their own timeslots

Page 6: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

6

Time Division

Mux

Tributaries are sent in their own timeslots

Tributaries are buffered and sent when capacity is available

Statistical Mux

What is a Wavelength Mux?

Page 7: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

7

Time Division

Mux

Tributaries are sent in their own timeslots

Tributaries are buffered and sent when capacity is available

Statistical Mux

Tributaries are sent over the same fibre, but at different wavelengths

Wavelength Division Mux

Tributaries may arrive on different fibres, and at "grey" wavelengths

Electrical inputs

What is a Wavelength Mux?

Page 8: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

8

Early WDM Deployment

• Two transmission wavelengths, most common... 1310nm 1550nm

• Coupler used to combine streams into the fibre

• Splitter (another coupler) and filters used to separate and detect specific streams

Page 9: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

9

Dense WDM

• Many more than 2 channels!• Initial ITU Grid allows 32 channels with 100GHz Spacing• Proprietary systems with up to 160 channels are

currently available as slideware

How many channels?

Be very, very careful regarding manufacturer claims!

(c.f. Never ask a barber if he thinks you need a haircut)

Be very, very careful regarding manufacturer claims!

(c.f. Never ask a barber if he thinks you need a haircut)

Page 10: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

10

Why don't the streamson different wavelengths

get "mixed up"?

Why don't the streamson different wavelengths

get "mixed up"?

Question...

Page 11: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

11

Dense WDM:ITU Channel Spacing

1600 1700140013001200 1500

Atte

nuat

ion

(dB

/km

)

Wavelength (nm)

0.1

0.2

0.3

0.4

0.5

0.6

15

25

15

30

15

35

15

40

15

45

15

50

15

55

15

60

15

65

ITU Channel Spacing 100GHz

(Currently)

ITU Channel Spacing 100GHz

(Currently)

Page 12: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

12

A Basic Answer

• Light is sent into the fibre on a very narrow range of wavelengths… A typical DFB laser peak width is ~10MHz (~1pm at 1500nm)

• Different channels are spaced so that they don't "overlap" In this context, "overlap" implies a power coupling (ie. interference)

between one channel and its neighbours Typical spacing "rule of thumb"…take the transmission rate in Gbps,

multiply by 2.5, and you have the minimum channel spacing in GHz (eg. 100GHz at 40Gbps)

Another "rule of thumb": each time you double the transmission rate or the number of channels, an additional 3dB of transmission budget is needed

• Need to know the range of available wavelengths in the fibre

Page 13: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

13

DWDM Channel Spacing

• Must have enough channel spacing to prevent interaction at a given transmission rate… 40Gbps 100GHz 10Gbps 25GHz 2.5Gbps 6GHz

• Must test lasers from large batch, ensure temperature stability, and include margins for component ageing

• Total range of wavelengths must be able to be consistently and reliably amplified by EDFA "Accepted" EDFA range is 1530 to 1565 nm (C-band)

• Must be aware of fibre limitations (see later)

Page 14: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

14

Why (and Where) DWDM?

• DWDM increases capacity on a given point to point linkBandwidth is multiplied by factor of 4, 8, 16 etc.

• Typical 1st generation DWDM is deployed in point to point topologies, over long-haul distances

• In Metro installations, there is an active debate between mesh and ring-based topologies

• Economics of Metro DWDM are not clear-cutOften is cheaper to deploy more fibre

These markets are… Changing rapidly Are sensitive to nature of installed fibre Are very sensitive to disruptive technologies

These markets are… Changing rapidly Are sensitive to nature of installed fibre Are very sensitive to disruptive technologies

…more later!

Page 15: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

15

DWDM Enabling Technologies

• The notion of "Service Transparency"• Laser sources• Receivers• Tuneable filters• Fibre gratings• Modulation and Modulators• Wavelength couplers and demuxers• Optical amplifiers• Points of flexibility

Optical Cross-Connect (OXC)

Optical Add-Drop Mux (OADM)

Page 16: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

16

Service Transparency

• Each Lambda can carry any serial digital service for which it has an appropriate physical interface SONET/SDH

Which can be carrying ATM, PoS and other services ESCON c.f. SCSI, which is a parallel communication channel

(parallel to serial converters are available for SCSI) Fast/Gigabit Ethernet

• Each channel can be transmitting at different rates

Page 17: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

17

Why Lasers?

• Lasers in general... High power output (compared to beam diameter) Narrow transmission spectrum High spatial quality beam (diffraction limited) Well-defined polarisation state

• Semiconductor lasers Small Size

To improve efficiency with fibre coupling

To allow high density port counts Industrial scale production

Needs lots of them!

Page 18: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

18

A Basic Semiconductor Laser

P

N

Reflective coating

Partially reflective coating

Page 19: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

19

How Do Lasers Work?

Electron

"Low" energy level

"High" energy level

Energy absorbed(pump)

Electron

"Low" energy level

"High" energy level

Energy emitted

Electrons exist in a stable "low" energy state until we pump in energy to promote

them to a higher state

High energy state is unstable and electron will soon decay back to the low energy state, giving out a characteristic level of

energy in the process

Characteristic energy

Page 20: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

20

A Laser Cavity

Reflective Surface

Reflective Surface

Atom in "high" energy state

Photon of characteristic energy

Atom in "low" energy state

Gain Medium

Atom will emit photon and return to "low" energy state.

The emitted photon has exactly the right energy to stimulate emission in the other high energy atoms

Photons that travel parallel to sides of resonant cavity are returned to stimulate further

emissions

Containment Layer

Electrodes

Page 21: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

21

Tuneable LasersWhat and Why?

• The ability to select the output wavelength of the laser… The primary sources are fixed wavelength

• What happens if one of these lasers fails? How many backup lasers would we need? What is the range of wavelengths over which we need to

operate?

• We could use one tuneable laser to back up all of the primary sources

Page 22: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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• There are three parameters that we trade-off in a tuneable laser… Tuning range (goal 35nm) Power output (goal 10mW) Settling latency (app. specific)

• Tunable lasers with a "slow" settling speed can be used in service restoration applications

• Tunable laser with a "fast" settling speed can also be used in next generation optical switching designs

Module 9831L Tuning Comb; Superimposed Spectra

-60

-55

-50

-45

-40

-35

-30

-25

-20

-15

-10

-5

0

1525 1530 1535 1540 1545 1550 1555 1560 1565 1570 1575

Wavelength (nm)

Ou

tpu

t (d

B r

el.)

Tuneable LasersWhat and Why?

Page 23: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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Signal Modulation

• Notion of imposing a digital signal on a carrier wave Amplitude Modulation Frequency Modulation Phase Modulation

• In Optical Communications, typically Amplitude Modulation NRZ and RZ encoding

• Directly modulated lasers• Externally modulated lasers

Page 24: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

24

Modulation Schemes

• NRZ: non-return to zero Most common modulation

scheme for short-medium-long haul

• RZ: return to zero Ultra-long haul

0 00

1 1Signal

1

0 00

1 1Signal

1

Page 25: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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A Traditional Optical Repeater

•High speed electrical componentsHigh cost, lower reliability

•Single wavelength operation•Regenerator will make amplifier rate-specific

This system is not Service-Transparent!This system is not Service-Transparent!

Page 26: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

26

OEO Amps in a DWDM System

RX

RX

RX

Amp

Amp

Amp

TX

TX

TX

TX

TX

TX

Amp

Amp

Amp

RX

RX

RX

~40km

Page 27: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

27

Solution:Broadband, All-Optical Amplifier

•Single amplifier for multiple wavelengths•No electrical components

Cheaper, more reliable, not rate-dependent

Gain elementGain element

Page 28: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

28

The EDFAWhat is "Erbium Doped"?

CoreCore

CladdingCladding

• Fibre is "doped" with the element Erbium Controlled level of Erbium introduced into silica core

and cladding

Page 29: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

29

The EDFAHow Does It Work?

• Energy is "pumped" into the fibre using a pump laser operating at 980nm

• Erbium acts as lasing medium, energy transferred to signal

• Not specific to wavelength (operates in the EDFA Window)

• Not specific to transmission rate

Page 30: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

30

The EDFAHow Does It Work?

Page 31: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

31

The EDFA WindowRegion of "flat gain"

OH-

OH-

OH-

Wavelength (nm)

700 800 900 1000 1100 1200 1300 1400 1500 1600 1700

Att

enu

atio

n (

dB

/km

)

0

1

2

3

4

5

First windowSecond windowThird windowFourth windowFifth window

EDFA Window: 1530-1565nm

Page 32: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

32

CWDM

Page 33: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

33

CWDM

Coarse wavelength division multiplexing (CWDM)

is a method of combining multiple signals on laser beams at various wavelenghts for transmission along fiber optic cables, such that the number of chanels is fewer than in dense wavelength division multiplexing (DWDM) but more than in standard wavelength division multiplexing (WDM).

Page 34: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

34

CWDM

CWDM systems have channels at wavelengths spaced 20 nanometers apart, compared with 0.4 nm spacing for DWDM. This allows the use of low-cost, uncooled lasers for CWDM.

In a typical CWDM system, laser emissions occur on eight channels at eight defined wavelengths:

1610 nm, 1590 nm, 1570 nm, 1550 nm, 1530 nm, 1510 nm, 1490 nm, 1470 nm.

But up to 18 different channels are allowed, with wavelengths ranging down to 1270 nm

Page 35: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

35

CWDM

Page 36: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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CWDM

Page 37: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

37

CWDM

System CWDMCoarse Wavelength Division Multiplexing

Page 38: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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CWDM

System CWDMCoarse Wavelength Division Multiplexing

Page 39: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

39

The Evolution of Fibre

• Fibre properties Attenuation Dispersion Non-linearlity

• Fibre Evolution Dispersion-Unshifted Fibre (USF) Dispersion-Shifted Fibre (DSF) Non-Zero Dispersion-Shifted Fibre (NZDF) Emerging fibre types

• Soliton Dispersion Management

Page 40: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

40

Optical Fibre Properties

Faster

Further

More Wavelengths

Traditional Challenges Fibre Properties Attenuation Modal Dispersion Chromatic Dispersion Polarisation Mode

Dispersion Non-linearity

» Self-phase modulation» Cross-phase

modulation» 4-wave mixing

Page 41: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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Fibre Optic PropertiesSignal Attenuation

OH-

OH-

OH-

~190THz

~50THz

Wavelength (nm)

700 800 900 1000 1100 1200 1300 1400 1500 1600 1700

Att

enu

atio

n (

dB

/km

)

0

1

2

3

4

5

First windowSecond windowThird windowFourth windowFifth window

1

2 3 45

Page 42: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

42

Fibre Optic PropertiesModal Dispersion

• In multimode cable, different modes travel at different speeds down the fibre

Result: signal is "smeared" Solution: single mode fibre

Signal in Signal out

Page 43: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

43

Fibre Optic PropertiesChromatic Dispersion

Different wavelengths travel at different speeds down the cable

Result: signal is "smeared" Solution: narrow spectrum lasers Solution: avoid modulation chirp Solution: dispersion management

Signal in Signal out

Page 44: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

44

Fibre Optic PropertiesPolarisation Mode Dispersion

Different polarisation components travel at different speeds down the cable

Result: signal is "smeared" Solution: design and installation experience, good test equipment

Slow

Fast PMD delay timePulses start journey in phase

After travelling down fibre, pulses are now

out of phase

Page 45: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

45

Fibre Optic PropertiesNon-Linear Effects

• Self Phase Modulation• Cross Phase Modulation• 4-Wave Mixing

Effects are "triggered" when power level of signal exceeds a

certain threshold

Page 46: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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Self Phase Modulation (SPM)

• Non-linear effect• Occurs in single and multi

wavelength systems In DWDM system, SPM will

occur within a single wavelength

• Two main effects… Spectral broadening Pulse compression

• Solution is positive dispersion in signal path In

ten

sity

Time

Spectral broadening

Page 47: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

47

Cross-Phase Modulation (XPM)

• Pulses in adjacent WDM channels exchange power ie. only happens in multi-

channel systems

• Primary effect is spectral broadening

• Combined with high dispersion, will produce temporal broadening

• Low levels of positive dispersion will help prevent inter-channel coupling

Page 48: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

48

Four Wave Mixing

Case 1: Intensity modulation between two primary channels at beat frequency

Result is two "phantom" wavelengths

Case 2: Interaction of three primary frequenciesResult is a "phantom" fourth wavelength

fF = fp + fq - fr

f1 f22f1-f2 2f2-f1fF

fp fq fr

Page 49: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

49

Fibre Evolution1st Generation: USF

1300 1400 1500 1600

-20

-10

0

10

20

Wavelength (nm)

Dis

per

sio

n (

ps/

nm

-km

)1310nm

Att

enu

atio

n (

dB

/km

)

0.2

0.3

0.4

0.5

Dispersion

USF

1550nm

Attenuation

Page 50: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

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Fibre Evolution2nd Generation: DSF

1300 1400 1500 1600

-20

-10

0

10

20

Wavelength (nm)

Dis

per

sio

n (

ps/

nm

-km

)

Att

enu

atio

n (

dB

/km

)

0.2

0.3

0.4

0.5

Dispersion

USF

DSF

Attenuation

1310nm 1550nm

Page 51: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

51

Fibre Evolution3nd Generation: NZDSF

1300 1400 1500 1600

-20

-10

0

10

20

Wavelength (nm)

Dis

per

sio

n (

ps/

nm

-km

)

Att

enu

atio

n (

dB

/km

)

0.2

0.3

0.4

0.5

Dispersion

USF

DSF

Attenuation

1310nm 1550nm

NZDF

Page 52: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

52

Next Generation Fibres...

• Remove OH- interaction to open 5th window Example: Lucent "All Wave" Fibre

• Minimise intrinsic PMD during manufacture PMD is the "2.5Gbps speed bump" Example: Corning LEAF PMD is very dependent on installation stresses

• Reduce loss at higher wavelengths (>1600nm) Selctive doping using chalcogenides

(Group VI elements) Fibre bend radius becomes significant

Page 53: 1 WDM Piotr Turowicz Poznan Supercomputing and Networking Center piotrek@man.poznan.pl 9-10 October 2006

53http://www.porta-http://www.porta-optica.orgoptica.org

Reichle & De-Massari

References